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A thermodynamic cycle with the highest efficiency is Carnot cycle. ηC =1−Tc (1) h In this ideal cycle compression and expansion are reversible and adiabatic and heat addition or rejection is isothermal. In real cycles all the attempts are concentrated to come closer to this condition. First improvement is usually to introduce heat regeneration. It lowers the heat addition as well as heat rejection according to formula for thermal efficiency: ηth =1−Qout =WT −WC (2) Qin Qin Methods such as split expansion with reheating or split compression with inter-cooling can increase thermal efficiency as well as net work but the cycle will became very complex and it has a negative effect on manufacturing, control, operating, maintenance, cost etc. An increase of turbine inlet temperature and pressure can be also applied but there are material limits. All methods may be combined in an effort to reach optimum solution but one has to aware of complex and uneconomic proposal. The analyzed cycles are: Simple Brayton cycle Pre-compression cycle Re-compression cycle Split expansion cycle Partial cooling cycle Partial cooling with improved regeneration 1.4 Simple Brayton cycle Figure 1.4 Simple Brayton cyclePDF Image | 2009 TECHNOLOGY INNOVATION WINNERS
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